Stellar black hole
Black holes formed from stellar collapse.
A stellar black hole, also called a stellar-mass black hole, forms when a star collapses under its own gravity. Its mass typically falls between about five and several tens of times the mass of the Sun. While many are the remnants of supernova explosions, other ways of forming them may exist.
According to the no-hair theorem, a black hole is defined by only three properties: mass, electric charge, and angular momentum. The angular momentum of a stellar black hole comes from the conservation of the spin of the star or objects that created it. A massive star inevitably collapses at the end of its life, once its internal energy sources are gone. If the collapsing core is below the Chandrasekhar limit, a white dwarf forms. If it is above that but below the Tolman–Oppenheimer–Volkoff (TOV) limit for neutron-degenerate matter, the result is a neutron star. If the collapsing core exceeds the TOV limit, the collapse continues until a black hole appears. These limits are approximate and can shift depending on the star's chemical makeup and rotation.
The exact maximum mass a neutron star can have before collapsing into a black hole is not fully known. In 1939, the TOV limit was estimated at 0.7 solar masses. By 1996, a different estimate placed the upper mass between 1.5 and 3 solar masses. The heaviest observed neutron star, PSR J0740+6620, discovered in September 2019, has a mass of about 2.14 solar masses.
In general relativity, a black hole could have any mass. The smaller the mass, the denser the matter must be to form one. No known stellar process produces black holes with masses less than a few times the Sun's mass; if such small black holes exist, they are likely primordial. Until 2016, the largest known stellar black hole had a mass of 15.65±1.45 solar masses. In September 2015, gravitational waves revealed a rotating black hole of 62±4 solar masses, formed when two smaller black holes merged. As of June 2020, the binary system 2MASS J05215658+4359220 contains the smallest known black hole, with a mass of 3.3 solar masses and a diameter of just 19.5 kilometers.
Observational evidence also points to two more massive types: intermediate-mass black holes in globular clusters and supermassive black holes at the centers of the Milky Way and other galaxies.
Stellar black holes in close binary systems become visible when matter flows from a companion star toward the black hole. The energy released as the matter falls heats it to hundreds of millions of degrees, producing X-rays. The black hole is thus seen in X-rays, while the companion star is observed with optical telescopes. The energy release is similar for black holes and neutron stars, making them hard to tell apart. Mass estimates come from observations of compact X-ray sources, combining X-ray and optical data. All known neutron stars have masses below 3.0 solar masses, and none of the compact systems above that mass show neutron star properties. This strongly suggests that compact objects above 3.0 solar masses in binaries are black holes. This proof is partly theoretical: no other object is known that could explain these massive compact systems. A direct proof would require observing the orbit of a particle or gas cloud falling into a black hole.
Some binaries are found far above the galactic plane due to black hole natal kicks. The velocity distribution of these kicks resembles that of neutron star kicks. One might expect the momenta to be similar, with black holes moving slower because they are heavier, but that does not appear to be the case. This may be because asymmetrically expelled matter falls back, increasing the black hole's momentum.
Some stellar evolution models predict that black holes cannot form directly from stellar collapse in two mass ranges: a "lower" gap of roughly 2 to 5 solar masses and an "upper" gap of about 50 to 150 solar masses (another estimate for the upper gap is 52 to 133 solar masses). A star's upper mass limit in the current universe is thought to be about 150 solar masses.
A lower mass gap is suspected because few candidates are observed with masses just above the maximum neutron star mass. The existence and theoretical basis for this gap are uncertain. Any black holes found in this range may have come from merging binary neutron stars rather than stellar collapse. The LIGO/Virgo collaboration reported three candidate events in their third observing run with component masses in this lower gap. There has also been a report of a bright, rapidly rotating giant star in a binary with an unseen companion that emits no light, including X-rays.
- mass_range
- 5 to several tens of solar masses
- formation
- gravitational collapse of a star
- key_properties
- mass, electric charge, angular momentum
- largest_known_mass_2016
- 15.65±1.45 solar masses
- largest_known_mass_2015_merger
- 62±4 solar masses
Lore & Background
Stellar black holes form when a massive star exhausts its nuclear fuel and undergoes gravitational collapse. If the collapsing core's mass exceeds the Tolman–Oppenheimer–Volkoff limit, collapse continues past the neutron star stage to form a black hole. Stellar black holes in close binary systems are observable when matter transferred from a companion star heats up to hundreds of millions of degrees and radiates X-rays. The black hole is detected in X-rays while the companion is seen optically. All identified neutron stars have mass below 3.0 solar masses, and none of the compact systems above that mass display neutron star properties, making it likely that such objects are black holes. The existence proof is not entirely observational but relies on theory, as no other object is known for these massive compact systems. Black hole natal kicks can propel binaries to large distances above the galactic plane. The velocity distribution of these kicks appears similar to that of neutron star kicks, contrary to expectations that higher mass would yield lower velocities. This may be due to fall-back of asymmetrically expelled matter increasing the black hole's momentum.
Reader's Guide
Stellar black holes are crucial for testing general relativity and understanding stellar evolution. They represent the endpoint of massive star life and provide natural laboratories for extreme gravity. Observations of X-ray binary systems allow mass measurements that distinguish black holes from neutron stars, with the 3.0 solar mass threshold serving as a practical dividing line. The existence of mass gaps—ranges where black holes are not expected to form directly from stellar collapse—challenges models and may be filled by merger products or other mechanisms. The smallest known stellar black hole, at 3.3 solar masses and 19.5 km diameter, pushes the lower boundary of observable masses. Their study continues to refine our understanding of compact object formation and the demographics of black holes in the universe.
Did You Know?
- All identified neutron stars have a mass below 3.0 solar masses, while compact systems above that mass are likely black holes.
Frequently Asked Questions
What is a stellar black hole?
A stellar black hole is the ultra-dense remnant left behind when a massive star's core collapses under its own gravity. It represents the endpoint of stellar evolution for stars that are too heavy to end as white dwarfs or neutron stars.
How are stellar black holes formed?
They come into being when a star's core can no longer resist gravitational pressure and undergoes a catastrophic collapse, often in the context of a supernova explosion. Other formation pathways beyond a simple supernova may also be at work, though the exact mechanisms are still being studied.
How do astronomers detect stellar black holes?
They are most often identified through X-ray emissions produced when the black hole pulls material off a companion star in a binary system. Gravitational-wave observatories also register the spacetime ripples generated when two stellar black holes spiral together and merge.
What properties define a stellar black hole?
Like every black hole, a stellar black hole is completely described by three parameters: its mass, its electric charge, and its angular momentum (spin). No additional internal detail is accessible to an outside observer, making these three numbers the full external signature of the object.
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